4.6 Article

Time Dependent Lyotropic Chromonic Textures in Microfluidic Confinements

期刊

CRYSTALS
卷 11, 期 1, 页码 -

出版社

MDPI
DOI: 10.3390/cryst11010035

关键词

lyotropic chromonic liquid crystals; microfluidics; surface anchoring; phase transition; herringbone; spherulite; textures

资金

  1. ATTRACT Investigator Grant of the Luxembourg National Research Fund [A17/MS/11572821/MBRACE]

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The nematic and columnar phases of lyotropic chromonic liquid crystals (LCLCs) have been extensively studied for their importance in material science and medical diagnostics. This study focuses on the emergence of time dependent textures in confined LCLCs, using soft lithography, surface characterization, and polarized optical imaging to analyze the confinement-induced LCLC textures. Varying confinement geometry, anchoring conditions, and initial DSCG concentration allows for tuning the temporal dynamics of the N- to M-phase transition and textural behavior of the confined LCLC.
Nematic and columnar phases of lyotropic chromonic liquid crystals (LCLCs) have been long studied for their fundamental and applied prospects in material science and medical diagnostics. LCLC phases represent different self-assembled states of disc-shaped molecules, held together by noncovalent interactions that lead to highly sensitive concentration and temperature dependent properties. Yet, microscale insights into confined LCLCs, specifically in the context of confinement geometry and surface properties, are lacking. Here, we report the emergence of time dependent textures in static disodium cromoglycate (DSCG) solutions, confined in PDMS-based microfluidic devices. We use a combination of soft lithography, surface characterization, and polarized optical imaging to generate and analyze the confinement-induced LCLC textures and demonstrate that over time, herringbone and spherulite textures emerge due to spontaneous nematic (N) to columnar M-phase transition, propagating from the LCLC-PDMS interface into the LCLC bulk. By varying the confinement geometry, anchoring conditions, and the initial DSCG concentration, we can systematically tune the temporal dynamics of the N- to M-phase transition and textural behavior of the confined LCLC. Overall, the time taken to change from nematic to the characteristic M-phase textures decreased as the confinement aspect ratio (width/depth) increased. For a given aspect ratio, the transition to the M-phase was generally faster in degenerate planar confinements, relative to the transition in homeotropic confinements. Since the static molecular states register the initial conditions for LC flows, the time dependent textures reported here suggest that the surface and confinement effects-even under static conditions-could be central in understanding the flow behavior of LCLCs and the associated transport properties of this versatile material.

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